The quantum phase transitions (continuous) at zero-temperature driven by
non-temperature parameters are believed to be key to understand some
unconventional properties of correlated many-body systems[1]}, [2]},
including strange metal phase in the high-temperature superconductors[3]}, [4]}, [5]},
ferromagnetic quantum criticality in the heavy fermion systems[6]} and deconfined quantum critical point (QCP)[7]}, [8]}.
From a field-theoretical perspective, the general description for the continuous phase transition can be formulated in terms of the order parameter which acquires a nonzero value as the system is tuned across the transition.
Together with the renormalization group (RG) theory[9]},
the Landau-Ginzburg-Wilson (LGW) paradigm provides a well understanding of the universal criticality and a effective method to calculate the critical exponents near the critical point, for example the extensively studied scalar \(O(N)\)  model which captures the continuous critical behavior of a wide variety of systems [2]}, [11]}, [12]}.
